Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana

Detalhes bibliográficos
Ano de defesa: 2009
Autor(a) principal: Otomar, Denilson Ramos
Orientador(a): Não Informado pela instituição
Banca de defesa: Não Informado pela instituição
Tipo de documento: Tese
Tipo de acesso: Acesso aberto
Idioma: por
Instituição de defesa: Programa de Pós-graduação em Física
Física
Programa de Pós-Graduação: Não Informado pela instituição
Departamento: Não Informado pela instituição
País: Não Informado pela instituição
Palavras-chave em Português:
Link de acesso: https://app.uff.br/riuff/handle/1/18638
Resumo: Elastic and quasi-elastic excitation functions for the 6,7 Li + 144 Sm systems were measured at backward angles for a range of energies from well below the barrier to above it. Moreover, barrier distributions were extracted from these excitation functions by a point difference method, using the first derivative of the excitation function. The analysis of the data was performed by using the code FRESCO, and the São Paulo potential as a parameter free bare one. From the analysis, on concluded that the inelastic excitations of 144 Sm are extremely relevant for that reactions in the absence o break-up channel. Furthermore, for the Li + 144 Sm reaction the nucleon transfer channel was included in the coupled scheme. An important point that must be taken into account is that, as no parameter of the São Paulo potential was changed, no attempt was made to fit the data, but rather, to compare the experimental excitation function and its corresponding barrier distribution with the theoretical predictions by using a coupling scheme that takes into account the above mentioned inelastic and transfers channels. This comparison for the excitation function gives reasonable good agreement, except at the higher energies. For the barrier distributions, one can notice more clearly that even at the barrier energy there is some disagreement between the experimental results and theoretical calculations. This discrepancy is not unexpected, since as Li are weakly bound projectile, one additional channel should also be included in the coupling scheme: the break-up channel. In order to verify the influence of the break-up channel in the quasi-elastic process, we performed calculations using the CDCC (Continuum Discretized Coupled Channels) method, since the break-up process feeds states in the continuum. In our calculations we assume the clusters model, which means that the Li break-up into deuteron and alpha particles. These clusters interact separately with the target before and after the ocurrence of the break-up. So, by adding this channel into the previously mentioned couple scheme, and excluding the transfer channel from coupling scheme of Li, the comparison the theoretical calculation with the experimental data gives rise to an excellent accuracy in the whole energy range for both the excitation function and the barrier distribution. It is important to mention that there were no fittings parameters in our calculation.
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spelling Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira CoulombianaBarrier distributions of 6,7 Li + 144 Sm systems at energies around the Coulomb barrierReação nuclearNuclear reactionCNPQ::CIENCIAS EXATAS E DA TERRA::FISICAElastic and quasi-elastic excitation functions for the 6,7 Li + 144 Sm systems were measured at backward angles for a range of energies from well below the barrier to above it. Moreover, barrier distributions were extracted from these excitation functions by a point difference method, using the first derivative of the excitation function. The analysis of the data was performed by using the code FRESCO, and the São Paulo potential as a parameter free bare one. From the analysis, on concluded that the inelastic excitations of 144 Sm are extremely relevant for that reactions in the absence o break-up channel. Furthermore, for the Li + 144 Sm reaction the nucleon transfer channel was included in the coupled scheme. An important point that must be taken into account is that, as no parameter of the São Paulo potential was changed, no attempt was made to fit the data, but rather, to compare the experimental excitation function and its corresponding barrier distribution with the theoretical predictions by using a coupling scheme that takes into account the above mentioned inelastic and transfers channels. This comparison for the excitation function gives reasonable good agreement, except at the higher energies. For the barrier distributions, one can notice more clearly that even at the barrier energy there is some disagreement between the experimental results and theoretical calculations. This discrepancy is not unexpected, since as Li are weakly bound projectile, one additional channel should also be included in the coupling scheme: the break-up channel. In order to verify the influence of the break-up channel in the quasi-elastic process, we performed calculations using the CDCC (Continuum Discretized Coupled Channels) method, since the break-up process feeds states in the continuum. In our calculations we assume the clusters model, which means that the Li break-up into deuteron and alpha particles. These clusters interact separately with the target before and after the ocurrence of the break-up. So, by adding this channel into the previously mentioned couple scheme, and excluding the transfer channel from coupling scheme of Li, the comparison the theoretical calculation with the experimental data gives rise to an excellent accuracy in the whole energy range for both the excitation function and the barrier distribution. It is important to mention that there were no fittings parameters in our calculation.Conselho Nacional de Desenvolvimento Cientifico e TecnológicoForam medidas funções de excitação elástica e quaseelástica para os sistemas 6,7Li +  144Sm para ângulos muito traseiros num intervalo de energia bem abaixo da barreira Coulombiana  até energias um pouco acima damesma. Empregando-se um método de diferença de pontos,  foram extraídas  distribição de barreira a partir da derivada primeira dessas  funções de excitação com relação à energia. A análise dos  dados experimentais foi feita utilizandose o código FRESCO e  tendo o potencial de São Paulo como potencial base.  A partir,então, da análise com o FRESCO, pudemos observar que as  excitações inelásticas (multipolar) do 144Sm são  extremamente relevantes nesta reação quando o canal de  breakup (quebra) não é incluído explicitamente. Além disso,  para a reação 7Li + 144Sm o canal de transferência de nucleons fora incluído nos cálculos. Um ponto importante a ser  salientado é que nenhum parâmetro do potencial de São Paulo foi mudado a fim de se ajustar os dados xperimentais. Ao  contrário, foram feitas comparações da função de excitação  experimental e a sua correspondente distribuição de barreira  com as previsões eóricas usando-se um esquema de acoplamento de canais que levou em conta os canais inelásticos e de transferências mencionados  acima. A comparação da função de excitação teórica com a  experimental fornece uma concordância muito boa, exceto na  região de alta energia. Para a distribuição de barreiras, pode-se notar mais claramente,  que mesmo na região da barreira  não há concordância entre os dados experimentais com as  previsões teóricas. Essa discrepância não é uma surpresa, pois, como se trata de uma reação onde os 6,7Li são projéteis fracamente ligados, deveríamos, então, incluir mais um canal  no esquema de acoplamentos: o canal de  break-up. Srndo assim, com o objetivo de verificar a influência desse  canal no processo quase elástico,  realizamos cálculos usando o método de CDCC. Tal  método faz-se necessário,  pois o canal de breakup popula estados no  contínuo.  Em nossos cálculos nós assumimos o modelo de  clusters, isto é, o 7Li quebrase em duas partículas,  trítio e alfa, enquanto o 6Li quebra-se em deuteron e alfa.  Estes clusters interagem com o alvo separadamente antes e  depois da quebra.  Somando-se então, o canal de breakup ao esquema de acoplameto descrito acima,  excetuando-se o canal de transferência no caso do 7Li,  a comparação dos cálculos teóricos com os dados experimentais fornece uma  concordância excelente em todo intervalo de energia anto  para a função de excitação quanto para distribuição de  barreira. Deve-se salientar que em nossos cálculos não existiu nenhum  parâmetro ajustável.        Programa de Pós-graduação em FísicaFísicaRíos, Jesús LubiánCPF:60111111122http://lattes.cnpq.br/9581543042568686Gomes, Paulo Roberto SilveiraCPF:60000101722http://lattes.cnpq.br/1265572757415786Otomar, Denilson Ramos2021-03-10T20:45:09Z2009-11-272021-03-10T20:45:09Z2009-02-15info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/doctoralThesisapplication/pdfhttps://app.uff.br/riuff/handle/1/18638porCC-BY-SAinfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da Universidade Federal Fluminense (RIUFF)instname:Universidade Federal Fluminense (UFF)instacron:UFF2021-03-10T20:45:09Zoai:app.uff.br:1/18638Repositório InstitucionalPUBhttps://app.uff.br/oai/requestriuff@id.uff.bropendoar:21202021-03-10T20:45:09Repositório Institucional da Universidade Federal Fluminense (RIUFF) - Universidade Federal Fluminense (UFF)false
dc.title.none.fl_str_mv Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
Barrier distributions of 6,7 Li + 144 Sm systems at energies around the Coulomb barrier
title Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
spellingShingle Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
Otomar, Denilson Ramos
Reação nuclear
Nuclear reaction
CNPQ::CIENCIAS EXATAS E DA TERRA::FISICA
title_short Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
title_full Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
title_fullStr Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
title_full_unstemmed Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
title_sort Distribuição de barreira dos sistemas 6,7Li + 144Sm em energias próximas à da barreira Coulombiana
author Otomar, Denilson Ramos
author_facet Otomar, Denilson Ramos
author_role author
dc.contributor.none.fl_str_mv Ríos, Jesús Lubián
CPF:60111111122
http://lattes.cnpq.br/9581543042568686
Gomes, Paulo Roberto Silveira
CPF:60000101722
http://lattes.cnpq.br/1265572757415786
dc.contributor.author.fl_str_mv Otomar, Denilson Ramos
dc.subject.por.fl_str_mv Reação nuclear
Nuclear reaction
CNPQ::CIENCIAS EXATAS E DA TERRA::FISICA
topic Reação nuclear
Nuclear reaction
CNPQ::CIENCIAS EXATAS E DA TERRA::FISICA
description Elastic and quasi-elastic excitation functions for the 6,7 Li + 144 Sm systems were measured at backward angles for a range of energies from well below the barrier to above it. Moreover, barrier distributions were extracted from these excitation functions by a point difference method, using the first derivative of the excitation function. The analysis of the data was performed by using the code FRESCO, and the São Paulo potential as a parameter free bare one. From the analysis, on concluded that the inelastic excitations of 144 Sm are extremely relevant for that reactions in the absence o break-up channel. Furthermore, for the Li + 144 Sm reaction the nucleon transfer channel was included in the coupled scheme. An important point that must be taken into account is that, as no parameter of the São Paulo potential was changed, no attempt was made to fit the data, but rather, to compare the experimental excitation function and its corresponding barrier distribution with the theoretical predictions by using a coupling scheme that takes into account the above mentioned inelastic and transfers channels. This comparison for the excitation function gives reasonable good agreement, except at the higher energies. For the barrier distributions, one can notice more clearly that even at the barrier energy there is some disagreement between the experimental results and theoretical calculations. This discrepancy is not unexpected, since as Li are weakly bound projectile, one additional channel should also be included in the coupling scheme: the break-up channel. In order to verify the influence of the break-up channel in the quasi-elastic process, we performed calculations using the CDCC (Continuum Discretized Coupled Channels) method, since the break-up process feeds states in the continuum. In our calculations we assume the clusters model, which means that the Li break-up into deuteron and alpha particles. These clusters interact separately with the target before and after the ocurrence of the break-up. So, by adding this channel into the previously mentioned couple scheme, and excluding the transfer channel from coupling scheme of Li, the comparison the theoretical calculation with the experimental data gives rise to an excellent accuracy in the whole energy range for both the excitation function and the barrier distribution. It is important to mention that there were no fittings parameters in our calculation.
publishDate 2009
dc.date.none.fl_str_mv 2009-11-27
2009-02-15
2021-03-10T20:45:09Z
2021-03-10T20:45:09Z
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/doctoralThesis
format doctoralThesis
status_str publishedVersion
dc.identifier.uri.fl_str_mv https://app.uff.br/riuff/handle/1/18638
url https://app.uff.br/riuff/handle/1/18638
dc.language.iso.fl_str_mv por
language por
dc.rights.driver.fl_str_mv CC-BY-SA
info:eu-repo/semantics/openAccess
rights_invalid_str_mv CC-BY-SA
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv application/pdf
dc.publisher.none.fl_str_mv Programa de Pós-graduação em Física
Física
publisher.none.fl_str_mv Programa de Pós-graduação em Física
Física
dc.source.none.fl_str_mv reponame:Repositório Institucional da Universidade Federal Fluminense (RIUFF)
instname:Universidade Federal Fluminense (UFF)
instacron:UFF
instname_str Universidade Federal Fluminense (UFF)
instacron_str UFF
institution UFF
reponame_str Repositório Institucional da Universidade Federal Fluminense (RIUFF)
collection Repositório Institucional da Universidade Federal Fluminense (RIUFF)
repository.name.fl_str_mv Repositório Institucional da Universidade Federal Fluminense (RIUFF) - Universidade Federal Fluminense (UFF)
repository.mail.fl_str_mv riuff@id.uff.br
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